which is the well known radial oscillator potential ( \(\omega >0,\ell >0\) ) whose
solutions [1]} are given in terms of the classical Laguerre polynomials
\(L^{(\ell +\frac{1}{2})}_{n}(z)\)
\(\tilde{\Psi }^{(1)}_{con,n}(r) = N^{\ell ,1}_{con,n}r^{\ell +1}\exp \bigg (-\frac{z(r)}{2}\bigg )L_{n}^{(\ell +\frac{1}{2})}(z(r)), \quad n=0,1,2,...\) 
